2001
DOI: 10.1063/1.1389514
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Traveling wave electro-optic phase modulators based on intrinsically polar self-assembled chromophoric superlattices

Abstract: Traveling-wave electro-optic modulators based on chromophoric self-assembled superlattices ͑SASs͒ possessing intrinsically polar microstructures have been designed and fabricated. Although the thickness of the SAS layer is only ϳ150 nm, a-phase shift is clearly observed. From the measured V value, the effective electro-optic coefficient of the SAS film is determined to be ϳ21.8 pm/V at an input wavelength of 1064 nm.

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Cited by 34 publications
(19 citation statements)
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“…An estimation of the r 33 coefficient corresponding to a d 33 value of 70 pm V ±1 gives r 33 = 38 pm V ±1 at 1064 nm, by considering e = 20, n = 1.5, and k max = 620 nm. [29,30] …”
Section: Poling Experiments and Nlo Propertiesmentioning
confidence: 99%
“…An estimation of the r 33 coefficient corresponding to a d 33 value of 70 pm V ±1 gives r 33 = 38 pm V ±1 at 1064 nm, by considering e = 20, n = 1.5, and k max = 620 nm. [29,30] …”
Section: Poling Experiments and Nlo Propertiesmentioning
confidence: 99%
“…Marks and coworkers. 43,44 Theoretical consideration of intermolecular interactions and exploitation of additional forces (ionic, hydrogen bonding) could conceivably permit significant improvement of this already promising approach.…”
Section: Molecular and Nanoscale Engineeringmentioning
confidence: 99%
“…Various implementations of this general structure include (1) chromophores physically incorporated into conventional polymers to form composite materials; (2) chromophores attached by a single bond (as a side chain) to a conventional polymer backbone (main chain); (3) chromophores incorporated into the backbone (main chain) of polymers; (4) chromophores attached by one end to a three-dimensional crosslinked polymer matrix; (5) chromophores attached at both ends to a 3D polymer matrix; (6) chromophores fabricated into ordered acentric lattices by sequential synthesis techniques based on exploiting ionic or covalent bonds; and (7) chromophores incorporated into crosslinked dendrimer structures. [12][13][14][15][16][43][44][45][46][47] Composite materials are the easiest to fabricate in that a chromophore can simply be dissolved in a commercially available polymer host material and poled near the glass transition temperature of the composite material. However, unless the glass transition temperature of the host polymer is above 150°C, poling induced acentric order will be quickly lost by rotational relaxation of the chromophores.…”
Section: Molecular and Nanoscale Engineeringmentioning
confidence: 99%
“…Additionally, these materials also exhibit a high optical transmission in the visible wavelength range, which facilitates optical measurements. 20,21 Also, from processing perspective, PMMA and PDMS substrates are often preferred materials. It is possible to fabricate two-or three-dimensional (2D or 3D) microfluidic geometries using rather straightforward micromachining processes.…”
Section: Fabrication Materialsmentioning
confidence: 99%